Determine the expectation value of the momentum of the particle. Explain.

Short Answer

Expert verified

The expected value of momentum is i1-a2a.

Step by step solution

01

Define expectation value

A particle of mass is represented by a wavefunction,

ψ(x)={2a3xe-axx>00x<0}

The expectation value ofA is defined as

A^=-ψ*xA^ψx

02

Determine the expectation value of momentum.

The expression for momentum operator is

p^=-ix

The expectation value of momentum is

p^=-ψ*xp^ψx=-i02a3xe-axx2a3xe-ax=-i02a3xe-ax2a3e-ax+xe-ax-a=ia02a3xe-ax2a3xe-ax-i02a3xe-ax2a3e-ax

Solve further as:

p^=ia0ψ2x-4a3i0xe-2ax

The integral in the first term will be equal to one as ψxis normalised. Solving integral in the second term separately as follows:

l=0xe-2ax=xe-2ax-2a-dxdxe-2ax=-xe-2ax2a-e-2ax4a20=14a2

Inserting this result in the above expression for momentum.

p^=ia-4a3i14a2=i1a-a=i1-a2a

The expected value of momentum is i1-a2a.

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Most popular questions from this chapter

Air is mostly N2, diatomic nitrogen, with an effective spring constant of 2.3 x 103N/m, and an effective oscillating mass of half the atomic mass. For roughly what temperatures should vibration contribute to its heat capacity?

Figure 5.15 shows that the allowed wave functions for a finite well whose depth U0was chosen to be6π2/mL2.

(a) Insert this value in equation (5-23), then using a calculator or computer, solve for the allowed value of kL, of which there are four.

(b) Usingk=2mEfind corresponding values of E. Do they appear to agree with figure 5.15?

(c) Show that the chosenU0implies that α12π2L2k2.

(d) DefiningLandCto be 1 for convenience, plug your KLand αvalues into the wave function given in exercise 46, then plot the results. ( Note: Your first and third KLvalues should correspond to even function of z, thus using the form withCOSKZ, while the second and forth correspond to odd functions. Do the plots also agree with Figure 5.15?

To show that the potential energy of finite well is U=h2(n1)28mL2

Show that the uncertainty in a particle’s position in an infinite well in the general case of arbitrary nis given by

L11212n2π2

Discuss the dependence. In what circumstance does it agree with the classical uncertainty of discussed in Exercise 55?

There are mathematical solutions to the Schrödinger equation for the finite well for any energy, and in fact. They can be made smooth everywhere. Guided by A Closer Look: Solving the Finite Well. Show this as follows:

(a) Don't throw out any mathematical solutions. That is in region Il (x<0), assume that (Ce+ax+De-ax), and in region III (x>L), assume thatψ(x)=Fe+ax+Ge-ax. Write the smoothness conditions.

(b) In Section 5.6. the smoothness conditions were combined to eliminate A,Band Gin favor of C. In the remaining equation. Ccanceled. leaving an equation involving only kand α, solvable for only certain values of E. Why can't this be done here?

(c) Our solution is smooth. What is still wrong with it physically?

(d) Show that

localid="1660137122940" D=12(B-kαA)andF=12e-αL[(A-Bkα)sin(kL)+(Akα+B)cos(kL)]

and that setting these offending coefficients to 0 reproduces quantization condition (5-22).

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